The comparison of optical and electronic properties between squarely and hexagonally arranged nano-porous layers and uniformly arranged nano-wired layers of aluminium and silver was presented. The nano-wired configuration exhibit 20 and 10% higher average transmittance in visible wavelength range in comparison to square and hexagonal nano-porous designs, respectively. The insignificant difference of the transmittance for aluminium and silver nano-porous and nano-wired layers is observed, when interpore/interwire distance is larger than wavelengths of incoming light. This difference becomes considerable at the interpore/interwire distance less than wavelengths of incoming light: silver nano-porous and nano-wired layers possess up to 27% higher transmittance in comparison to aluminium layers.

Formation of thin-film nanomaterials, promising for nanoelectronic applications, with a given structure based on octa-phenyl-2,3-naphthalocyaninato zinc.

One-step cost effective process of fabrication of a full inorganic nanostructured transparent conductive electrode and LC alignment layer has been developed. More specifically, the subject comprises a self-organized nanomesh of a valve metal, concomitant porous oxide layer with various functionality and electrochemical method of their fabrication. The nanomesh film is electrically conductive, optically transparent and flexible. It can be fabricated on a variety of substrates, including flexible and rigid substrates. High effective LC alignment layers based of nanostructured alumina can be fabricated at the same anodization process by special electro-chemical technique in sulfuric and oxalic acids to form a self ordered nanoporous structure of alumina which has a "vertical" surface area that prevails over the "horizontal" one even though Al film's thickness is small. The possibility to control distances between pores and their sizes during the process of anodizing/etching enables to optimize alignment surface according to the required LC material.

. Moreover, alternative TCLs should be preferably flexible and have low cost. Different materials such as carbon nanotubes [4,5], graphene layers [6,7], zinc oxides [8], organic polymers [9], ultra thin metallic layers [10,11] and metallic nanogratings [12][13][14][15] were proposed as possible TCL candidates. But so far none of them has been adopted to replace the ITO [4][5][6][7][8][9]. Thin metallic layers of 10-50 nm thickness are the simplest flexible TCLs which can transmit up to 50% of incoming light in the visible spectrum [16]. Modifying these metallic layers to nanogratings can improve their opto-electronic performance up to that of ITO [14,[17][18][19][20]. The fabrication process of nanogratings includes lithography, nanoimprinting, and solution-processing. This paper presents a nonlithographic method of the fabrication of nanoporous Al TCLs. The transparent conductive nanomesh (or nanograting) was made by electrochemical anodizing of Al

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In this paper, we describe the new concept of design, synthesis, and application of nanostructured anisotropic materials and conductive and alignment coatings for high efficient displays and photonic devices. It is based on the original combination of anisotropic and nanostructured materials, conductive and alignment coatings, and includes the design and synthesis of new anisotropic materials and the preparation of novel conductive and alignment coatings.

Получены плавающие слои и пленки Ленгмюра-Шеффера субфталоцианина бора A 2 B типа. Построены модели face-on и edge-on монослоевых упаковок исследуемого соединения на поверхности раздела фаз воздух/вода и рассчитаны геометрические характеристики данных упаковок. Установлено, что площадь, приходящаяся на одну молекулу в плотнейшем face-on монослое, равна 1,99 нм 2 (А мол = 1,99 нм 2 ), edge-on монослое -1,02 нм 2 (А мол = 1,02 нм 2 ). Изучены спектральные характеристики исследуемого соединения в хлороформе и в пленках Ленгмюра-Шеффера. В спектре пленки Ленгмюра-Шеффера по сравнению со спектром раствора в хлороформе полосы поглощения смещены в длинноволновую область и незначительно уширены. Данные изменения спектров пленок Ленгмюра-Шеффера мы объясняем наличием межмолекулярных π-π взаимодействий push-pull молекул субфталоцианина в этих пленках и хаотическим расположением агрегатов в них. Методом атомно-силовой микроскопии установлена толщина перенесенной пленки (d = 0,7 нм).Ключевые слова: субфталоцианин, модель надмолекулярной упаковки, плавающие слои, пленки Ленгмюра-Шеффера, атомно-силовая микроскопия, оптические свойства.

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